The discussion explores whether the solution of the wave equation can be expressed as f=g[(±)ct(±)x]. It demonstrates that this form satisfies the wave equation by deriving the first and second derivatives with respect to both space and time. The analysis confirms that the function is differentiable, continuous, and defined at all points, which are essential conditions for double differentiation. The conclusion emphasizes that these properties validate the proposed solution form. The explanation aims to clarify any doubts regarding the wave equation's solution.